Electro-Magnetic Strong Force: String Theory without the String
Date: 2010-11-20 Time: 07:00 - 09:00 US/Pacific (1 decade 4 years ago)
America/Los Angeles: 2010-11-20 07:00 (DST)
America/New York: 2010-11-20 10:00 (DST)
America/Sao Paulo: 2010-11-20 11:00
Europe/London: 2010-11-20 14:00
Asia/Colombo: 2010-11-20 19:30
Australia/Sydney: 2010-11-21 01:00 (DST)
Where: Online Video Conference
Recording Playback
This video conference used DimDim, now a private company.
The meeting can be replayed by clicking this link:
watch the meeting recording
This video conference used DimDim, now a private company.
The meeting can be replayed by clicking this link:
watch the meeting recording
Description
I propose and algorithmically derive an alternative color model to that of the RGB and CMYK models, and provide the mathematical reasons why those models are comparably insufficient. This model directly connects with our perceived colors and matches their known frequencies in SI units, as well as experimental observation. More importantly, it carries throughout the electro-magnetic spectrum where no modern model does, toward both the infrared and ultraviolet frequencies. Once this basis is made, I derive an inseparable connection between the nuclear strong force and the primary function of this model. It has long been observed that the sub-atomic particles comprising the nuclear particles behave in ways that resemble the "additive" and "subtraction" nature of colored lens combinations, but I show that this behavior it neither additive nor subtractive in reality, rather algebraic, and that this behavior is not only analogous, but required. I provide examples, evidence and mathematics that demonstrate how this process works from numerous perspectives not only for the electro-magnetic spectrum, but also the electro-magnetic field itself. The results reveal how the Nuclear Strong force is better described with electro-magnetism than with the notion of a string or gluon and that white light cannot be comprised of all the colors or the spectrum, as Newton supposed, rather, a non-tonal aspect of a light wave with no phase angle shifts.